The Higgs trilinear coupling λ hhh is of great importance to understand the structure of the Higgs sector and allows searching for indirect signs of Beyond-the-Standard-Model (BSM) physics, even if new states are somehow hidden. In particular, in models with extended Higgs sectors, it is known that non-decouplings effects in BSM-scalar contributions at one loop can cause λ hhh to deviate significantly from its SM prediction, raising the question of what happens at two loops. We review here our calculation [1, 2] of the leading two-loop corrections to λ hhh in an aligned scenario of a Two-Higgs-Doublet Model. We find their typical size to be 10-20% of the one-loop corrections, meaning that they do not modify significantly the one-loop non-decoupling effects, but are not entirely negligible either.
I. INTRODUCTIONThe discovery of the 125-GeV Higgs boson at the CERN LHC in 2012 has been a great success for particle physics, and has completed the particle spectrum of the Standard Model (SM). However, while it is now established that the Higgs sector is responsible for the electroweak symmetry breaking (EWSB), very little is known about the nature of the Higgs potential -in fact, only its minimum and the curvature around the minimum are known. Moreover, although some new physics must exist -possibly not too far from the electroweak (EW) scale -to address shortcomings of the SM, there is so far no clear sign of it in experiments. A first possible explanation for this could be that new physics only exists beyond the scale currently accessible at colliders, and hence their effects would be (almost) impossible to find. Another interesting possibility would be that the new states are made somehow difficult to observe via some symmetry or mechanism.A prime example of the latter is alignment [3], which is defined for models of several Higgs doublets as the limit in which the total EW vacuum expectation value (VEV) is colinear in field a Speaker.